Biomedical Engineering Reference
In-Depth Information
is the random variable counting those tips which are born in A
.
By definition
d
Φ ( {
0
R
)=
N 0 . This process
Φ
is characterized by the following stochastic
intensity:
d
μ (
d t
×
d x
)=
prob
( Φ (
d t
×
d x
)=
1
|F t )= Λ t (
d x
)
d t
,
for
(
t
,
x
,
s
) R + × R
.
F t
denotes the
σ
algebra history of the process up to time t
and, given a
d
nonnegative function h
C b (R
)
and
α R + ,
t )
i = 1 ε X i ( t ) ( d x ) .
N
(
Λ t (
d x
)= α
h
(
C
(
t
,
x
))
(9)
When a tip located in x branches at time t , the initial value of the state of the new
tip is taken as
X N ( t )+ 1
v N ( t )+ 1
(
,
)=(
x
,
v 0 )
,where v 0 is a non random velocity and
T N ( t )+ 1 =
t . Given the branching process
Φ
, the counting process N
(
t
)= Φ ([
0
,
t
] ×
d
R
is a Poisson-like stochastic process, counting the total number of cells born
before t
)
R + , with intensity
N
)
i = 1 h ( C ( t , X i
(
t
d
ν (
d t
)= Λ t (R
)
d t
=
(
t
)))
d t
.
Evolution of the Fields. The chemotactic field C
diffuses and degrades; the
consumption is proportional to the extension velocities v i
(
t
,
x
)
,
i
=
1
,...,
N
(
t
)
.So,for
d ,
any
(
t
,
x
) R + × R
N ( t )
i = 1 ( v i
1
N
t C
(
t
,
x
)=
c 1 δ A (
x
)+
c 2
C
(
t
,
x
)
c 3 C
(
t
,
x
)
(
t
) δ X i
)
K N )(
x
) .
(10)
(
t
c 3 R + in Eq. ( 10 ) represent the rate of production of a source
located in a region A
Parameters c 1 ,
c 2 ,
d , modelling, e.g., a tumor mass, the diffusivity and the
rate of consumption, respectively.
Fibronectin is known to be attached to the extracellular matrix and does not
diffuse [ 2 ], thus the equation for fibronectin does not contain any diffusion term.
As in [ 36 ], degradation of fibronectin, characterized by a coefficient
R
β 2 , depends
on the concentration of MDE, produced by the cells. Hence, the concentration of
fibronectin f
(
x
,
t
)
produced by the endothelial cells at the tip evolves as
N
)
i = 1 ( δ X i ( t ) K N )( x ) β 2 m ( t , x ) f ( t , x ) ,
(
t
)= β 1 1
N
f
(
t
,
x
(11)
t
for
β 1 , β 2 R + . The MDE, once produced with rate
ν 1 , diffuses locally with
diffusion coefficient
ε 1 and is spontaneously degraded at a rate
ν 2 .
 
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